Nature 464, 80-84 (4 March 2010) | doi:10.1038/nature08813; Received 22 September 2009; Accepted 7 January 2010

Reinventing germanium avalanche photodetector for nanophotonic on-chip optical interconnects

Solomon Assefa1, Fengnian Xia1 & Yurii A. Vlasov1

  1. IBM T. J. Watson Research Center, Yorktown Heights, New York 10598, USA

Correspondence to: Solomon Assefa1 Correspondence and requests for materials should be addressed to S.A. (Email: sassefa@us.ibm.com).

Integration of optical communication circuits directly into high-performance microprocessor chips can enable extremely powerful computer systems1. A germanium photodetector that can be monolithically integrated with silicon transistor technology2, 3, 4, 5, 6, 7, 8 is viewed as a key element in connecting chip components with infrared optical signals. Such a device should have the capability to detect very-low-power optical signals at very high speed. Although germanium avalanche photodetectors9, 10 (APD) using charge amplification close to avalanche breakdown can achieve high gain and thus detect low-power optical signals, they are universally considered to suffer from an intolerably high amplification noise characteristic of germanium11. High gain with low excess noise has been demonstrated using a germanium layer only for detection of light signals, with amplification taking place in a separate silicon layer12. However, the relatively thick semiconductor layers that are required in such structures limit APD speeds to about 10GHz, and require excessively high bias voltages of around 25V (ref. 12). Here we show how nanophotonic and nanoelectronic engineering aimed at shaping optical and electrical fields on the nanometre scale within a germanium amplification layer can overcome the otherwise intrinsically poor noise characteristics, achieving a dramatic reduction of amplification noise by over 70 per cent. By generating strongly non-uniform electric fields, the region of impact ionization in germanium is reduced to just 30nm, allowing the device to benefit from the noise reduction effects13, 14, 15 that arise at these small distances. Furthermore, the smallness of the APDs means that a bias voltage of only 1.5V is required to achieve an avalanche gain of over 10dB with operational speeds exceeding 30GHz. Monolithic integration of such a device into computer chips might enable applications beyond computer optical interconnects1—in telecommunications16, secure quantum key distribution17, and subthreshold ultralow-power transistors18.


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